Abstract:In this paper the general question of laser-induced photochemistry on metal surfaces is addressed. Specifically, we have studied resonant photodecomposition of a variety of aromatic molecules on roughened silver surfaces in ultrahigh vacuum. A continuous ion laser source at a number of different wavelengths in the region 350-410 nm was used to produce graphitic carbon on the surface which was monitored by Raman spectroscopy at the 1580-cm"1 band of surface carbon. Laser power-dependence studies of fragmentatio… Show more
“…Additionally, interference between the incident, transmitted, and reflected radiation was not taken into account (12). No pronounced surface-enhanced photodissociation was seen, as has been reported for rough metal surfaces (36,37) and for OCS on unannealed LiF(OO1) (1 2a,b). We also note that the QMS samples a small solid angle (-5.5"), while for accurate cross section measurements all particles must be detected, i.e., angular distributions may vary with coverage, as noted by Polanyi and co-workers (9).…”
Section: Photodissociatiorz Cross Section Of Adsorbed Clnosupporting
Can. J. Chem. 72,737 (1994). The 365 nm pulsed laser photolysis of nitrosyl chloride adsorbed on a rough MgO(100) surface at 90 K has been studied. Mass spectrometric detection was used to record time-of-flight (TOF) spectra by monitoring Cl' and NO' . These ions can derive from parent ClNO, which fragments completely in the mass spectrometer, as well as from C1 and NO photofragments. The TOF distributions are considerably slower than for the corresponding gas phase photodissociation process. NO was also detected state selectively by using resonance enhanced multiphoton ionization (REMPI), and a channel corresponding to direct adsorbate photolysis was identified. The state selective detection of NO molecules that emerge from the surface following photolysis shows unambiguously that their rotational degrees of freedom reflect the surface temperature (Trot = 100-140 K), even at low coverages. At similar photolysis wavelengths, gas phase ClNO photodissociation is known to produce highly rotationally excited NO with a distinctive non-statistical distribution peaked at J" = 46.5. Our studies suggest that, contrary to the gas-phase photolysis results, C1 and NO are not ejected rapidly following photolysis of surface-bound species on a repulsive potential energy surface. We postulate that ClNO grows in islands, with MgO defect sites serving as nucleation centers. Photofragment rotational and translational excitations are quenched efficiently due to strong attractive interactions that equilibrate NO to the surface temperature. Desorption of intact ClNO may also take place, but following (i.e., not during) the photolysis pulse. Such desorbed species can contribute to the TOF spectra, but not the REMPI spectra.L. HODGSON, G. ZIEGLER, H. FERKEL, H. REISLER et C. WIT~IG. Can. J. Chem. 72,737 (1994).OpCrant B 90 K, on a CtudiC la photolyse B 365 nm, par laser pulsC, du chlorure de nitrosyle adsorb6 sur du MgO(100) rugueux.On a utilisC la detection par spectromCtrie de masse en temps de vol (TOF) pour dCtecter le C1' et le NO' . Ces ions peuvent provenir du ClNO parent qui se fragmente completement dans le spectre de masse ainsi que des photofragments Cl et NO. Les distributions dans les spectres en TOF sont beaucoup plus lentes que dans le cas du processus correspondant de photodissociation en phase gazeuse. On a aussi dCtectC ~Clectivement divers Ctats du NO en faisant appel B la rksonance par ionisation multiphotonique amCliorCe (REMPI) et on a identifit un canal correspondant B une photolyse directe de la substance adsorbee. La detection selective d'ttats des molCcules de NO qui Cmergent de la surface B la suite de la photolyse dtmontre sans ambigu'itC que leurs degres de libertC de rotation sont des reflets de la tempCrature B la surface (Trot = 100-140 K), mEme B de faibles taux de couverture. A des longueurs d'onde de photolyse semblables, il est connu que la photodissociation en phase gazeuse de ClNO conduit h du NO dont l'excitation rotationnelle est ClevCe et qui prCsente une distribution non-statistique distinctive...
“…Additionally, interference between the incident, transmitted, and reflected radiation was not taken into account (12). No pronounced surface-enhanced photodissociation was seen, as has been reported for rough metal surfaces (36,37) and for OCS on unannealed LiF(OO1) (1 2a,b). We also note that the QMS samples a small solid angle (-5.5"), while for accurate cross section measurements all particles must be detected, i.e., angular distributions may vary with coverage, as noted by Polanyi and co-workers (9).…”
Section: Photodissociatiorz Cross Section Of Adsorbed Clnosupporting
Can. J. Chem. 72,737 (1994). The 365 nm pulsed laser photolysis of nitrosyl chloride adsorbed on a rough MgO(100) surface at 90 K has been studied. Mass spectrometric detection was used to record time-of-flight (TOF) spectra by monitoring Cl' and NO' . These ions can derive from parent ClNO, which fragments completely in the mass spectrometer, as well as from C1 and NO photofragments. The TOF distributions are considerably slower than for the corresponding gas phase photodissociation process. NO was also detected state selectively by using resonance enhanced multiphoton ionization (REMPI), and a channel corresponding to direct adsorbate photolysis was identified. The state selective detection of NO molecules that emerge from the surface following photolysis shows unambiguously that their rotational degrees of freedom reflect the surface temperature (Trot = 100-140 K), even at low coverages. At similar photolysis wavelengths, gas phase ClNO photodissociation is known to produce highly rotationally excited NO with a distinctive non-statistical distribution peaked at J" = 46.5. Our studies suggest that, contrary to the gas-phase photolysis results, C1 and NO are not ejected rapidly following photolysis of surface-bound species on a repulsive potential energy surface. We postulate that ClNO grows in islands, with MgO defect sites serving as nucleation centers. Photofragment rotational and translational excitations are quenched efficiently due to strong attractive interactions that equilibrate NO to the surface temperature. Desorption of intact ClNO may also take place, but following (i.e., not during) the photolysis pulse. Such desorbed species can contribute to the TOF spectra, but not the REMPI spectra.L. HODGSON, G. ZIEGLER, H. FERKEL, H. REISLER et C. WIT~IG. Can. J. Chem. 72,737 (1994).OpCrant B 90 K, on a CtudiC la photolyse B 365 nm, par laser pulsC, du chlorure de nitrosyle adsorb6 sur du MgO(100) rugueux.On a utilisC la detection par spectromCtrie de masse en temps de vol (TOF) pour dCtecter le C1' et le NO' . Ces ions peuvent provenir du ClNO parent qui se fragmente completement dans le spectre de masse ainsi que des photofragments Cl et NO. Les distributions dans les spectres en TOF sont beaucoup plus lentes que dans le cas du processus correspondant de photodissociation en phase gazeuse. On a aussi dCtectC ~Clectivement divers Ctats du NO en faisant appel B la rksonance par ionisation multiphotonique amCliorCe (REMPI) et on a identifit un canal correspondant B une photolyse directe de la substance adsorbee. La detection selective d'ttats des molCcules de NO qui Cmergent de la surface B la suite de la photolyse dtmontre sans ambigu'itC que leurs degres de libertC de rotation sont des reflets de la tempCrature B la surface (Trot = 100-140 K), mEme B de faibles taux de couverture. A des longueurs d'onde de photolyse semblables, il est connu que la photodissociation en phase gazeuse de ClNO conduit h du NO dont l'excitation rotationnelle est ClevCe et qui prCsente une distribution non-statistique distinctive...
“…In this regard, in particular, the nanoscale control of the Au film structure is crucial towards the determination of its properties in view of applications in functional nano-devices. For example, the roughness of deposited metal films is one of the most critical determining final electrical, optical and other properties of the systems [16][17][18][19][20][21][22][23][24][25]. As examples: (a) one of the key issue in the modern integrated circuit technology is the dramatic increase in metallic interconnect resistivity with decreasing cross section thickness.…”
Section: Introductionmentioning
confidence: 99%
“…As a consequence, the roughness determines the absorbing and scattering properties of the metal film. By controlling these properties, thin metal films are exploited as light absorbing or scattering elements in plasmonic solar cells or other optical devices [20][21][22][23]; (d) laser-induced photochemistry on metal surfaces is widely studied as an effective means to catalyze surface reactions for specific adsorbates [24]. However, the surface roughness of the metal film was proved to greatly impacts on the rate of the reactions by controlling the light absorption in the metal film; (e) surface roughness dictates, also, the surfaces wetting properties and its nanoscale control is essential for designing and controlling wetting processes in general.…”
Deposited Au films and coatings are, nowadays, routinely used as active or passive elements in several innovative electronic, optoelectronic, sensing, and energy devices. In these devices, the physical properties of the Au films are strongly determined by the films nanoscale structure. In addition, in these devices, often, a layer of Ti is employed to promote adhesion and, so, influencing the nanoscale structure of the deposited Au film. In this work, we present experimental analysis on the nanoscale cross-section and surface morphology of Au films deposited on Ti. In particular, we sputter-deposited thick (>100 nm thickness) Au films on Ti foils and we used Scanning Electron Microscopy to analyze the films cross-sectional and surface morphology as a function of the Au film thickness and deposition angle. In addition, we analyzed the Au films surface morphology by Atomic Force Microscopy which allowed quantifying the films surface roughness versus the film thickness and deposition angle. The results establish a relation between the Au films cross-sectional and surface morphologies and surface roughness to the film thickness and deposition angle. These results allow setting a general working framework to obtain Au films on Ti with specific morphological and topographic properties for desired applications in which the Ti adhesion layer is needed for Au.
“…Photodecomposition of pyridine and other aromatic molecules on roughened Ag(110) surfaces has also been attributed to an enhanced two-photon absorption process. 12 Much larger enhancements of nonlinear optical effects and TPA, in particular, are expected to occur near fractal clusters of metal nanoparticles. 4 Because an applied electromagnetic field can excite collective oscillations of free electrons (plasmons) of metal nanostructures, large local fields can be generated.…”
Strong enhancement of the two-photon absorption of organic molecules near silver nanoparticle fractal clusters has been observed and has been exploited to yield composite materials with very strong two-photon absorption and two-photon-excited fluorescence properties. Measurements on cluster films coated with chromophoric polymer or with thiol-bound chromophores give spatially-averaged enhancements of 1000 and 20 000, respectively. Two-photon fluorescence microscopy studies show that the enhancements are spatially inhomogeneous, with peak-enhancement factors of g 10 000 (polymer/cluster) and g 160 000 (thiol chromophore/cluster), and excitation frequency dependent. These results are in accord with theoretical predictions of local-field effects due to strong localization of collective plasmon modes in fractal metal clusters, and demonstrate an approach to ultrasensitive two-photon processes.
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